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Another type of photoactivated mass migration system has been rst proposed by Ubukata (Ubukata et al., 2000) and extended by Zettsu and coworkers (Zettsu and Seki, 2004; Zettsu et al., 2001), using soft LC polymer systems such as binary component materials and random copolymers containing an oligo(ethylene oxide) (EO) segment (Fig. 8.9). The hybrid lms are irradiated with nonpolarized UV (365 nm) light in advance to attain a cis-rich photoequilibrated state (UV light treatment). Starting from this state, an argon ion laser beam (488 nm) or a 436-nm line from a mercury lamp, which induces the isomerization to the trans form, is irradiated to the lm. The mass migration is completed at surprisingly small dose levels (o100 mJ cm 2), which are three orders of magnitude smaller than those required for the conventional amorphous polymer systems. This fact strongly suggests that the migration mechanism of this type fully differs from that of the conventional type. A very recent study revealed that the photochemical phase change (Ikeda, 2003) of the smectic LC to isotropic phase is essential for the migration (Zettsu et al., 2007a). Therefore, this class of materials can be dubbed as the phase transition (PT) type. c# ean 128 reader Packages matching GS1-128 - NuGet Gallery
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Apr 22, 2018 · Decode EAN-128 with ByteScout Barcode Reader SDK https://bytescout.com/articles ...Duration: 0:58 Posted: Apr 22, 2018 With regard to the migration mechanisms for the conventional type, a number of models have been proposed. The details are discussed in the literatures (Natansohn and Rochon, 2002; Sekkat and Knoll, 2002; Yager and Barrett, 2001; Viswanathan et al., 1999). In the conventional type, considerations of electromagnetic force given by photons seem to explain the migration behavior most appropriately. For the PT type, however, no summary has been reported. Therefore, a brief summary will be made here. The properties of the PT-type motions together with those of the conventional type are summarized in Table 8.1. There are a number of different issues in the migration feature for the two types. The mass migration of PT type has no polarization dependence, which shows a marked contrast with the conventional type. Two beam experiments show that the (p-:p-) (intensity and polarization holography) and (s-:s-) (pure intensity holography) mode interference equally cause the ef cient migration, but (s-:p-) mode (pure polarization holography) does not lead to any surface relief formation (Zettsu et al., 2003) (Fig. 8.10). Other notable features in the PT type are the occurrences of continuing motions even after ceasing the illumination (Ubukata et al., 2004), and migrations are also promoted via sensitized excitation from a near infrared absorbing dye (Zettsu et al., 2007a). In these contexts, the essence of the migration in the PT type should be thermal processes via self-assembly of the lm material, and the electromagnetic c# gs1 128 ilopez/GS1Parser: A GS1 Parser for C - GitHub
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